Skip to main content
banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
The full text of this article is not currently available.
/content/aip/journal/jmp/20/9/10.1063/1.524289
1.
1.D. Lovelock, “Divergence‐Free Third Order Concomitants of the Metric Tensor in Three Dimensions,” in Topics in Differential Geometry, edited by H. Rund and W. F. Forbes (Academic, New York, 1976), p. 87.
2.
2.For notation see S. J. Aldersley, Phys. Rev. D 15, 370 (1977).
2.The definition of a tensorial concomitant used here is that on p. 35 of Ref. 9 in G. W. Horndeski, Utilitas Math. 9, 3 (1976). For example, a scalar density concomitant of a pseudo‐Riemannian metric is defined by a real‐valued function φ of the form The concomitant φ is said to be of class provided the function φ is of class at every metric in its domain. (For example, and are of class but is only continuous since it is not differentiable in any neighborhood of a metric for which at some point).
3.
3.E. Cotton, “Sur les varietés à trois dimensions,” Ann. Fac. d. Sc. Toulouse (11) 1, 385 (1899).
4.
4.J. W. York has used this tensor density with reference to the initial‐value problem in general relativity. See Phys. Rev. Lett. 26, 1656 (1971),
4.and C. W. Misner, K. S. Thome, and J. A. Wheeler, Gravitation (Freeman, San Francisco, 1973), pp. 541 and 550.
5.
5.If then .
6.
6.G. W. Horndeski, Tensor 28, 303 (1974).
7.
7.I. M. Anderson Aeq. Math, (to be published). Also see Ref. 11.
8.
8.K. Kuchař [J. Math. Phys. 15, 708 (1974)] has considered the tensor density and shown that it is not an Euler‐Lagrange expression. [Note that is not symmetric unless one is constrained to metrics for which Hence the fact that for any L is obvious.] His method of proof does not apply to the Cotton tensor density in view of Eqs. (4) and the existence of a Lagrangian of the form (5). (That is, the functional curl of the Cotton tensor density vanishes identically).
9.
9.T. Y. Thomas, The Differential Invariants of Generalized Spaces (Cambridge U.P., Cambridge, 1934), p. 109.
10.
10.H. Weyl, The Classical Groups (Princeton U.P., Princeton, 1939), p. 52 noting p. 65.
11.
11.These points are discussed further in S. J. Aldersley, “High Euler Operators and some of their Applications,” preprint available from the author.
12.
12.J. W. York, J. Math. Phys. 14, 456 (1973).
13.
13.Generalizations of the Cotton tensor density for higher dimensional spaces will be discussed in S. J. Aldersley and G. W. Horndeski (in preparation).
http://aip.metastore.ingenta.com/content/aip/journal/jmp/20/9/10.1063/1.524289
Loading
/content/aip/journal/jmp/20/9/10.1063/1.524289
Loading

Data & Media loading...

Loading

Article metrics loading...

/content/aip/journal/jmp/20/9/10.1063/1.524289
2008-07-29
2016-09-28
Loading

Full text loading...

true

Access Key

  • FFree Content
  • OAOpen Access Content
  • SSubscribed Content
  • TFree Trial Content
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
/content/realmedia?fmt=ahah&adPositionList=
&advertTargetUrl=//oascentral.aip.org/RealMedia/ads/&sitePageValue=jmp.aip.org/20/9/10.1063/1.524289&pageURL=http://scitation.aip.org/content/aip/journal/jmp/20/9/10.1063/1.524289'
Right1,Right2,Right3,